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‫فرع السيراميك ومواد البناء‬/‫المرحلة الثالثة‬
Characteristic of Ceramic Materials/mechanical properties
1. Deformation
1-1. ELASTICITY
Elasticity can be seen by a reduction, at least partial, of the deformation when
the load applied on a body is released. From ambient temperature (or below) and up
to relatively high temperatures (T < 1,000°C), ceramics are elastic materials par
excellence: their behavior under load is most often linear with a nearly full
reversibility of the deformation on removal of the load and the fracture takes place
during elastic loading (no plasticity), for a deformation less than 1%. Refractories are
generally of mixed nature, ionic and covalent. It is difficult to deform these. In
covalent crystals (for example B4C or Si3N4) this is due to the directivity of the
bonds, while in ionic crystals (for example NaCl or ZrO 2) it is due to deep
disturbances in the electrostatic interactions resulting during the deformation of the
crystal. All interatomic forces are electrostatic in origin. The simplest expression for
the bond energy is
(1.1)
Where r is the interatomic distance and A, B, n, and m are constants characteristic
of the type of bonding. The first term is the attractive component the second is due to
repulsion. Only when m>n will a minimum (equilibrium) value of E is possible.
Equation 1.1 indicates that attractive forces predominate when atoms are far apart and
repulsive interactions predominate when the atoms are close together. The bond–
energy curve can be plotted as shown in Figure 1.1a. When the energy is a minimum
the atoms are at their equilibrium separation (r=r0); the lowest energy state defines
the equilibrium condition. In discussing ceramics, we usually think of the material in
terms of ions; ions with the same sign always repel one another due to the Coulomb
force. If we differentiate Eq. 1.1 with respect to r, we obtain an equation that
describes the resultant force F between a
(1.2)
The force will be zero at the equilibrium separation. The sign conventions for force,
In Figure 1.1a the force is attractive when F is positive. This is the usual convention
in materials science (and in Newton’s law of universal gravitation). The force is
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‫فرع السيراميك ومواد البناء‬/‫المرحلة الثالثة‬
Characteristic of Ceramic Materials/mechanical properties
attractive if A >0 and negative if A <0. Beware: in electrostatics, the convention is
that a negative force is attractive.
FIGURE 1.1 (a) Bond-energy curve for KCl. At infinite separation, the energy is that required
to form K
-distance curves for two
materials: one where the bonding is strong and one where it is weak.
1-1.1 YOUNG’S MODULUS
We can change the equilibrium spacing (r0) of the atoms in a solid by applying
a force. We can push the atoms closer together (compression), r >r0, or pull them
further apart (tension), r <r0. Young’s modulus (E) is a measure of the resistance to
small changes in the separation of adjacent atoms. It is the same for both tension and
compression.
Young’s modulus is related to the interatomic bonding forces and, as you might
expect, its magnitude depends on the slope of the force–distance curve at r0.
Close to r0 the force–distance curve approximates a tangent; when the applied forces
are small the displacement of the atoms is small and proportional to the force.
We can define the stiffness of the bond, S0, as the slope of this line:
(1.3)
The stiffness is analogous to the spring constant or elastic force constant of a spring
and is the physical origin of Hooke’s law. Close to r0 we can assume that the force
between two atoms that have been stretched apart a small distance r is
(1.4)
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‫فرع السيراميك ومواد البناء‬/‫المرحلة الثالثة‬
Characteristic of Ceramic Materials/mechanical properties
If we consider pulling two planes of atoms apart then the total force per unit area
can be obtained by dividing F by r20
(1.5)
Where σ and ε they are stress and strain, respectively. Moduli obtained from this
approach are approximate because they relate to two atoms only, ignoring the effects
of neighboring atoms. As the interatomic spacing, and in some cases the bonding,
Young’s modulus is dependent upon the
varies with direction in a single crystal,
direction of stress in relation to the crystal axes. Single crystals are elastically
anisotropic.
Figure 1.1b shows force–distance plots for two materials; one having weakly
bonded atoms and the other having strongly bonded atoms. With reference to bond–
energy curves a material with a high modulus will have a narrow, steep potential
energy well; a broad, shallow energy well would be characteristic of a low modulus.
Table 1.1 lists values of Young’s moduli for different materials as a function of
melting temperature. You can see the general trend: the higher the melting
temperature, the higher the modulus. Melting temperatures are also indicative of bond
strengths, which are determined mainly by the depth of the energy well. The modulus
is determined by the curvature at the bottom of the well. It is this difference that
accounts for deviations from the general trend. As the temperature of a material is
increased it is generally found that Young’s modulus slowly decreases as shown for
single-crystal aluminum oxide (corundum) in Figure 1.2. As we approach absolute
zero, the slope of the curve approaches zero as required by the third law of
thermodynamics. An empirical relationship that fits the data for several ceramics is
(1.6)
E0 is Young’s modulus at absolute zero and b and T0 are empirical constants; T0 is
about half the Debye temperature. (The Debye temperature is the temperature at
which the elastic vibration frequency of the atoms in a solid is the maximum.) As the
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‫فرع السيراميك ومواد البناء‬/‫المرحلة الثالثة‬
Characteristic of Ceramic Materials/mechanical properties
temperature is increased the separation between the atoms is increased and the force
necessary for further increases is slightly decreased.
For polycrystalline ceramics there is an additional effect due to grain boundaries.
At high temperatures there is a rapid decrease in the measured values of Young’s
moduli, this has been attributed to non elastic effects such as grain boundary sliding
and grain boundary softening. So Young’s modulus of a bulk ceramic is continuing to
change as described by Eq. 1.5,
FIGURE 1.2 Temperature dependence of
Young’s modulus for corundum.
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